Tunable impedance surface

• US 6,483,480 B1
• Filed: 06/08/2000
• Issued: 11/19/2002
• Est. Priority Date: 03/29/2000
• Status: Expired due to Term

• Current Assignee: HRL Laboratories LLC (The Boeing Co.)
• Original Assignee: HRL Laboratories LLC (The Boeing Co.)
• Inventors: Schaffner, James H., Sievenpiper, Daniel, Loo, Robert Y., Tangonan, Greg
• Primary Examiner(s): PHAN, THO GIA
• Application Number:
  US09/589,859
• Time in Patent Office: 894 Days
• Field of Search: H01/Q 1.502, 343/700.MS, 343/754, 343/756, 343/778, 343/850, 343/853, 343/909, 343/910
• US Class Current: 343/909
• CPC Class Codes: H01H 59/0009 making use of micromechanics
• CPC Class Codes: H01Q 15/0066 said selective devices being reconfigurable, tunable or controllable, e.g. using switches
• CPC Class Codes: H01Q 15/008 said selective devices having Sievenpipers' mushroom elements
• CPC Class Codes: H01Q 3/44 varying the electric or magnetic characteristics of reflecting, refracting, or diffracting devices associated with the radiating element
• CPC Class Codes: H01Q 9/0442 with particular tuning means

Abstract

A tuneable impedance surface for steering and/or focusing a radio frequency beam. The tunable surface comprises a ground plane; a first plurality of elements disposed in an array a first distance from the ground plane, the distance being less than a wavelength of the radio frequency beam; and a second plurality of elements disposed in an array a second distance from the ground plane, the second plurality of elements be moveable relative to the first plurality of elements.

Claims

1. A tuneable impedance surface for reflecting a radio frequency beam, the tunable surface comprising:

(a) a ground plane;

(b) a first plurality of elements disposed in an array a first distance from the ground plane, the distance being less than a wavelength of the radio frequency beam; and

(c) a second plurality of elements disposed in an array a-second distance from the ground plane, the second plurality of elements being moveable relative to the first plurality of elements.

2. The tuneable impedance surface of claim 1 further including a first substrate having first and second major surfaces, said substrate supporting said ground plane on the first major surface thereof and supporting said first plurality of elements on the second major surface thereof.

3. The tuneable impedance surface of claim 1 further including a second substrate having first and second major surfaces, said substrate supporting said second plurality of elements on the second major surface thereof.

4. The tuneable impedance surface of claim 3 wherein each element of the first and second pluralities of elements has an outside dimension which is less than the wavelength of the radio frequency beam.

5. The tuneable impedance surface of claim 1 wherein the first plurality of elements is coupled to the ground plane by electrically conductive vias in a substrate supporting said ground plane and said first plurality of elements.

6. The tuneable impedance surface of claim 1 wherein the first plurality of elements is arranged in a planar array.

7. The tuneable impedance surface of claim 1 wherein the second plurality of elements is arranged in a planar array.

8. The tuneable impedance surface of claim 1 wherein the first plurality of elements and the second plurality of elements are separated by a dielectric layer.

9. The tuneable impedance surface of claim 8 wherein the first plurality of elements and the second plurality of elements abut said dielectric layer.

10. The tuneable impedance surface of claim 8 wherein the first plurality of elements is fixed relative to said dielectric layer and the second plurality of elements is moveable relative to said dielectric layer.

11. The tunable tunable impedance surface of claim 1 wherein the first plurality of elements are disposed in a two dimensional array, wherein each of the first plurality of elements are spaced from one another, wherein the second plurality of elements are disposed in a two dimensional array, wherein each of the second plurality of elements are spaced from one another and wherein the second plurality of elements are disposed between the first plurality of elements and the ground plane.

12. A method of tuning a high impedance surface for reflecting a radio frequency signal comprising:

arranging a first plurality of spaced-apart conductive surfaces in an array disposed essentially parallel to and spaced from a conductive back plane,

arranging a second plurality of spaced-apart conductive surfaces in an array disposed essentially parallel to and spaced from said conductive back plane by a distance greater than the distance said first plurality of spaced-apart conductive surfaces is spaced from said conductive back plane, and

moving the second plurality of spaced-apart conductive surfaces relative to the first plurality of spaced-apart conductive surfaces.

13. The method of claim 12 wherein said pluralities of spaced-apart conductive surfaces are arranged on a printed circuit board.

14. The method of claim 12 wherein the step of moving the second plurality of spaced-apart conductive surfaces relative to the first plurality of spaced-apart conductive, surfaces comprises rotational movement in a plane essentially parallel to said arrays.

15. The method of claim 12 wherein the size of each conductive surface along a major axis thereof is less than a wavelength of the radio frequency signal, and preferably less than one tenth of a wavelength of the radio frequency signal, and the spacing of each conductive surface of the first plurality from the back plane is less than a wavelength of the radio frequency signal.

16. The method of claim 12 wherein the high impedance surface is tuned so that a generally linear reflection phase function is impressed on the high impedance surface.

17. The method of claim 16 wherein the linear phase function has discontinuities of 2π

therein.

18. The method of claim 12 wherein the conductive surfaces are generally planar and wherein the array is generally planar.

19. The method of claim 12 wherein the conductive surfaces are metallic and wherein the conductive back plane is metallic.

20. The method of claim 12 wherein the size of each conductive surface along a major axis thereof is less than one tenth of a wavelength of the radio frequency signal and the spacing of each conductive surface of the first plurality from the back plane is less than a wavelength of the radio frequency signal.

21. A tuneable impedance surface for reflecting a radio frequency beam, the tunable surface comprising:

(a) a first substrate formed of a dielectric material having a thickness which is less than a wavelength of the radio frequency beam;

(b) a conductive plane disposed on a major surface of said first substrate;

(c) a first plurality of conductive elements disposed in an array on another major surface of said first substrate, wherein each element of the first plurality of elements has an outside dimension which is less than the wavelength of the radio frequency beam;

(d) a second substrate disposed (i) in a confronting relationship to said first substrate and (ii) relatively moveable to said first substrate; and

(e) a second plurality of conductive elements disposed in an array on said second substrate wherein each element of the second plurality of elements has an outside dimension which is less than the wavelength of the radio frequency beam.

22. The tuneable impedance surface of claim 21 wherein the first plurality of elements are coupled to the conductive plane by electrically conductive vias arranged in said first substrate.

23. A tuneable impedance surface for reflecting a radio frequency beam impinging the tuneable impedance surface, the tunable surface comprising:

(a) a ground plane;

(b) a first plurality of elements disposed in a two dimensional array a first distance from the ground plane, the distance being less than a wavelength of the radio frequency beam; and

(c) a second plurality of elements disposed in a two dimensional array a second distance from the ground plane, the second plurality of elements being disposed adjacent to and moveable relative to the first plurality of elements for changing a direction by which the radio frequency signal reflects from the high impedance surface.

24. The tunable tunable impedance surface of claim 23 wherein each of the first plurality of elements are spaced from one another, wherein each of the second plurality of elements are spaced from one another and wherein the second plurality of elements are disposed between the first plurality of elements and the ground plane.

25. The tunable tunable impedance surface of claim 24 wherein the first plurality of elements are arranged on a first substrate, wherein the first plurality of elements are ohmically isolated from one another on the first substrate, wherein the second plurality of elements are arranged on a second substrate, and wherein the second plurality of elements are ohmically isolated from one another on the second substrate.

26. A method of tuning a high impedance surface for reflecting a radio frequency signal impinging the high impedance surface, comprising:

arranging a first plurality of spaced-apart, isolated conductive surfaces in a two dimensional array disposed essentially parallel to and spaced from a conductive back plane,

arranging a second plurality of spaced-apart, isolated conductive surfaces in a two dimensional array disposed essentially parallel to and spaced from said conductive back plane by a distance greater than the distance said first plurality of spaced-apart conductive surfaces is spaced from said conductive back plane, and

moving the second plurality of spaced-apart conductive surfaces relative to the first plurality of spaced-apart conductive surfaces in order to change a direction by which the radio frequency signal reflects from the high impedance surface.